In
fluid dynamics
In physics and engineering, fluid dynamics is a subdiscipline of fluid mechanics that describes the flow of fluids— liquids and gases. It has several subdisciplines, including ''aerodynamics'' (the study of air and other gases in motion) an ...
, a moving shock is a
shock wave that is travelling through a
fluid
In physics, a fluid is a liquid, gas, or other material that continuously deforms (''flows'') under an applied shear stress, or external force. They have zero shear modulus, or, in simpler terms, are substances which cannot resist any shear ...
(often
gaseous) medium with a
velocity relative to the velocity of the fluid already making up the medium.
[Shapiro, Ascher H., ''Dynamics and Thermodynamics of Compressible Fluid Flow,'' Krieger Pub. Co; Reprint ed., with corrections (June 1983), .] As such, the
normal shock relations require modification to calculate the properties before and after the moving shock. A knowledge of moving shocks is important for studying the phenomena surrounding
detonation, among other applications.
Theory
To derive the theoretical equations for a moving shock, one may start by denoting the region in front of the shock as subscript 1, with the subscript 2 defining the region behind the shock. This is shown in the figure, with the shock wave propagating to the right.
The velocity of the gas is denoted by ''u'',
pressure by ''p'', and the local
speed of sound
The speed of sound is the distance travelled per unit of time by a sound wave as it propagates through an elastic medium. At , the speed of sound in air is about , or one kilometre in or one mile in . It depends strongly on temperature as w ...
by ''a''.
The speed of the shock wave relative to the gas is ''W'', making the total velocity equal to ''u
1'' + ''W''.
Next, suppose a
reference frame is then fixed to the shock so it appears stationary as the gas in regions 1 and 2 move with a velocity relative to it. Redefining region 1 as ''x'' and region 2 as ''y'' leads to the following shock-relative velocities:
:
:
With these shock-relative velocities, the properties of the regions before and after the shock can be defined below introducing the
temperature as ''T'', the
density as ''ρ'', and the
Mach number
Mach number (M or Ma) (; ) is a dimensionless quantity in fluid dynamics representing the ratio of flow velocity past a boundary to the local speed of sound.
It is named after the Moravian physicist and philosopher Ernst Mach.
: \mathrm = \frac ...
as ''M'':
:
:
:
:
Introducing the
heat capacity ratio as ''γ'', the
speed of sound
The speed of sound is the distance travelled per unit of time by a sound wave as it propagates through an elastic medium. At , the speed of sound in air is about , or one kilometre in or one mile in . It depends strongly on temperature as w ...
, density, and pressure ratios can be derived:
:
:
:
One must keep in mind that the above equations are for a shock wave moving towards the right. For a shock moving towards the left, the ''x'' and ''y'' subscripts must be switched and:
:
:
See also
*
Shock wave
*
Oblique shock
*
Normal shock
*
Gas dynamics
*
Compressible flow
*
Bow shock (aerodynamics)
*
Prandtl-Meyer expansion fan
References
{{Reflist
External links
NASA Beginner's Guide to Compressible Aerodynamics
Fluid dynamics
Aerodynamics
Shock waves